Radiant energy – Infrared-to-visible imaging – Including detector array
Reexamination Certificate
1997-08-26
2001-02-06
Ham, Seungsook (Department: 2878)
Radiant energy
Infrared-to-visible imaging
Including detector array
C250S208100, C250S252100
Reexamination Certificate
active
06184527
ABSTRACT:
TECHNICAL FIELD OF THE INVENTION
The present invention relates generally to infrared detectors, and more particularly to a method of compensating for non uniformities among detector elements of an infrared detector array.
BACKGROUND OF THE INVENTION
Infrared detectors provide thermal images for temperature measurement and heat detection. They are used for various applications, such as for military, industrial, and medical applications. In its simplest form, an infrared detector is a device, such as a photosensitive diode, that generates an electric current when exposed to infrared radiation. This current is dependent on the intensity and wavelength of the radiation and can be used in many different ways to produce an infrared picture.
Infrared detectors may be configured as a single element (detector), a small array of elements, a long linear array, or a full two-dimensional array. When the detector is a full two-dimensional array, the entire image is recorded at once, and the array is referred to as a “staring” array. However, with smaller arrays, the image is scanned over the array. The small array requires a serial scan to sweep the image in two-dimensions, whereas the linear array requires a “pushbroom” scan to sweep the image across the array in one dimension.
The current produced by an infrared detector is amplified and processed to provide a more useful detector output. The processing reduces interference due to external and internal causes, such as electrical noise.
The ideal response of an infrared detector array is that each detector element exhibit the same linear voltage response for given temperature changes in the irradiation of the array. However, one type interference with a good detector signal is electrical noise due to detector non-uniformity among detector elements. The uniformity differences have both spatially and temporally dependent causes.
A number of methods have been tried for compensating non uniformity of infrared detector arrays. Generally, all involve some sort of data processing. Some methods use a uniform calibration source, typically using a chopper and controlled temperature. Other methods are scene-based, which means that they use an image comprised of one or more objects or patterns. The scene-based methods may be further categorized into mechanical and non-mechanical methods.
The “dithered scan” method of non uniformity compensation is a scene-based mechanical method. The detector array views a scene through suitable optics. During a given time frame, the incident flux is sensed by each detector element. At the end of the time frame, the array data is delivered for processing and the array is displaced (“dithered”) a fixed distance, typicallly a distance equal to the width or height of one detector element, in either the horizontal or vertical direction. The scene flux is assumed-to be stable throughout the dither cycle. Thus, during the next time frame, each detector element is exposed to the flux seen by one of its neighbors during the prior time frame. These detector pairs can be “linked” analytically, such as by averaging their outputs. By a suitable choice of a dither pattern, each detector can be linked with several of its neighbors, to adjust gain and offset differences. A dithered scan approach is described in an article by William F. O'Neil, “Dithered Scan Detector Compensation”,
Proc. IRIS Passive Detectors,
1992, Vol. 1, pp. 123-134.
SUMMARY OF THE INVENTION
One aspect of the invention is a method of calculating gain correction values to compensate gain errors of detector elements of an infrared detector array, using a dither pattern of said array, where the dither steps have a dither bias. A maximum gradiant of the scene being detected is determined. For a current detector element, a gain ratio of neighboring detector elements is calculated, these neighboring detector elements having dither paths parallel to the direction of the maximum gradient. The gain ratios are averaged, thereby obtaining a gain correction value for the current detector element. These calculating and averaging steps are repeated for additional sets of neighboring detector elements, thereby determing a gain correction value for each detector element of the array.
Thus, as indicated by the above method, the basic dithered gain correction calculations are modified for dither bias. Other modifications may be made for scene motion. Offset correction calculations may also be modified for dither bias and scene motion. Interpolation methods may be used for partial pixel dithering, where the dither step is different from the pixel dimension.
REFERENCES:
patent: 5514865 (1996-05-01), O'Neil
patent: 5526021 (1996-06-01), Naylor, Jr.
patent: 5712685 (1998-01-01), Dumas
Dithered Scan Detector Compensation, W.F. O'Neil, Proc. IRIS Passive Sensors, vol. 1, 1992.
Baker & Botts L.L.P.
Ham Seungsook
Hanig Richard
Raytheon Company
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